Method for making high-frequency cable joints



Feb. 14, 1950 1 WETHERILL 2,497,707

METHOD FOR MAKING HIGH-FREQUENCY CABLE JomTs Original Fled Feb. 2l, 1945 2 She'ets-Shee't, l

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inventor: Lgnn VVeGlwevii7 His .t'tovn eg.

Feb. 14, 1950 L. wETHr-:RILL

METHOD FOR MAKING H1GH-FREQUENCY CABLE Joms 2 Sheets-Sheet 2 Original Filed' Feb. 21, 1945 "R lm I ll.. l B uw M Anm@ ou asm @am P.

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Lghn -Wethevlh bis M fsx/ttowneg Patented Feb. 14, 1950 METHOD FOR MAKING HIGH-FREQUENCY CABLE J OINTS Lynn Wetherill, Pittsfield, Mass., assignor to General Electric Company, a corporation of New York Original application February 21, 1945, Serial No. 578,965. Divided and this application May 15,

1946, Serial No. 669,857

2 Claims.

My invention relates to electric cable joints in the form of connectors for making joints between lengths of various types of cable. More speccally, the invention relates to methods for constructing connectors for cables which are particularly adapted for the transmission of high 5 iointin which the refraction of a high frequency frequency currents of the order of several hunwave at the joint is so controlled as to reduce died megacycles. This application is a division reeCtiOnS t0 a minimum of my copending application for Electric cable It is a further object of my invention to proand cable joint, Serial No. 578,965, iiled Februvide anew and improved method 0f fastening the ary 21, 1945, and assigned to the same assignee connector of a cable joint structure to the as the instant application. severed end of the cable which method may be My invention is of particular interest in conemplOyed equally Weilv in the field aS in the nection with cables having solid dielectric mefaCtOrydium between the inner and outer conductors in In the accompanying drawing, Flg 1 liluSe which lengths of the cable are connected to trates a cable and a joint therefor constructed in other cables by means of connectors employing aCeOrdanCe with my inVentiOn; Figs- 2 and 3 dinerent dielectric medium from that used in the illustrate successive steps in the method of form-A cable. Sometimes joints using a solid dielectric ing the Cable J'Oint; Fig. 4 illustrates a modificamedium may be used but usually the medium is 2o tiOn 0f the Cable forming method; Fig. 5 illusgaseous, such as air. One advantage of using trates apparatus fOr Carrying Out the methodair as the dielectric medium at tue cable joint according to my invention; Fig. 6 is an explodedv is that it permits quick assembling and disman- View of parts of the apparatus of Fig- 5, and tling of such cable connections in field use. At Figs. 7, 8 and 9 are diagrammatic VieWS illus'- the same time, the connection er joint between treting the principles by which electric energy is cable sections must be so constructed that the transmitted threugh a high frequency Cable and' separable parts thereof may be quickly and easily J'Oint Constructed aCCOrding t0 my inventionattached to lengths of cable cut from bulk stock'. It iS Weil knOWn that the Characteristie im- It is of particular importance in cable lengths pedanee, 0r Surge impedance, Z 0f an eleetrie used with high frequency currents that the char- 3c Cable or of any small part thereof may be eX acteristic impedance, oi' surge impedance, of the Dressed aSv cable be uniform throughout its. length irre- L spective of variations in the dielectric media used Z =`f in adjacent sections of cable, and in the joints connecting these sections, and irrespective of 111 Willh variations in the diameters of the inner and outer L=inductance in hemies per unit length conductors. Such variations in diameters al-y Czcapacitance nfarads per unit length. most invariably occur at pointswhere joints are placed in the cable length in order to secure uni-l Thls'term may also be expressed as form breakdown strength in the dielectric me- 40 z w60 l R dium. s E OBV;

The requirement of constant surge impedance alone will not sufce to give highest eiliciency in in which' e high frequency transmission line incorporating k=dieiectric constant of the insulating medium joints. I have found that it is also important to between the inner and outer conductors. so construct the cable joint that no reflection of R.'=inner diameter of the outer conductor and the high frequency waves occurs at faces ber=outer diameter ofthe inner conductor. tween diierent dielectric media, particularly From this formula, it Will be seen that thev where the diameters of the inner and outer characteristic impedance of the cable is a funcconductors have been changed as at the cable tion of-three-variables k, R, and r. If any one ofjoint. Otherwise, spurious or unwanted standing waves may result with consequent loss of power in the transmission line.

It is an object of my invention to provide a new and improved method of constructing a cable 3 these variables is changed, a corresponding change will be necessary in the remaining variables if the characteristic impedance of the cable is to be maintained constant throughout its length.

In cases where it is desired to utilize cable joints having separable connectors for taking lengths of cable apart, provision must be made for connecting together the inner and outer conductors of the cable length. This means that some form of connector must be fastened to the inner conductor.

inner conductor of the high frequency cable. Furthermore, it is highly desirable to employ a gas insulating medium, such as air, at the cable joint so that no diiiculty will be experienced in taking the joint apart in field use. be seen that if the equation logs stant of about 2.4. Furthermore, I have chosen `to illustrate such a cable as being provided with connectors forming a cable joint in which air is utilized as a gaseous dielectric medium between the inner and outer conductors. The dielectric constantof air is 1. Since the dielectric constant of air is less than that of polyethylene, the ratio R/ r in the joint must be smaller than for the cable. Since dielectric strength of air is less than that of polyethylene, the spacing between the conductors at the joint must be increased in order not to lower the overall dielectric strength of the cable. However, the diameters of the inner and outer conductors of the cable have been so chosen in relation to the dielectric medium as to make the characteristic impedance of the joint substantially equal to that of the cable. In order to match the characteristic or surge impedance of the joint to that of the cable, and in order to connect the large diameter conductors of the joint to the relatively smaller conductors of the cable, a portion of the joint is formed with tapered conductors so that the diameters and spacing of the conductors of the cable are gradually increased to those of the joint. This arrangement is shown by Fig. 1.

Although the characteristic impedance of the joint has been matched to that of the cable, this requirement alone is not sufficient to attain maximum efficiency in the transmission line. It is also important to so construct the cable joint that no reflections of high frequency waves occur as the wave passes down the cable. Heretofore,

the dielectric medium in the cable has been tere'- minated abruptly whenever the cable has been connected to a'joint having a different dielectric medium. This has almost invariably resulted in reflection of part of the wave in those instances in which there is a change in the diameters of the inner and outer conductors at cable joints. However, I have found that the interface between the two dielectric mediums of the cable and joint Almost invariably the connector is of a diameter greater than that of the` It will thus may be so positioned as to substantially preclude reflections of the high frequency wave and at the same time give a substantially constant surge impedance at the joint. The wave is refracted so that it passes from one dielectric medium to the other with substantially no reection. The arrangement is particularly useful in those instances in which the diameter of the cable joint varies from that of the cable and in which tapered conductors are used in the joint to obtain a uniform characteristic impedance of the transmission line.

In Fig. 1 of the drawing, I have shown a cable and joint therefor in which a portion of the solid dielectric of the cable has been extended up into the cable joint and terminated at an interface or boundary disposed at an angle. This angle is critical. It depends upon the dielectric constants of the insulating materials used in the cable and joint. It is so located as to keep the characteristic impedance of the cable substantially constant through the joint as well as precluding reflections of the high frequency wave. In order to more fully explain the manner in which the angle of the boundary is determined, I have shown the arrangement of the dielectric media and boundary in the diagrammatic views of Figures 8 and 9.

In Figure 8, the high frequency wave is represented as parallel lines moving along the paths of the dielectric media. It remains as nearly as possible perpendicular to the boundaries formed by the conducting surfaces. The wave is shown moving along the solid dielectric until it reaches the boundary where it is refracted as it passes into the gaseous dielectric medium. As mentioned above, the boundary angle is critical in order to secure proper refraction of the wave. In order to illustrate the boundary angle, a small portion of the wave front and boundary angle, as indicated by the dotted lines in Fig. 8, have been shown in the enlarged schematic view of Fig. 7.

Fig. 'I illustrates the boundary plane separating the two dielectric media which are indicated by the parallel dotted lines. The dotted lines also represent the path of the high frequency wave. In Figure '7,

B=angle of incidence of the wave A=angle of refraction of the wave. It is assumed that V1=Velocty of wave in insulating material entering boundary V2=velocity of wave in insulating material leaving boundary.

By the sine law of refraction Since the velocity of an electric wave is inversely proportional to the square root of the dielectric constant 1 Vl-T;

where K1=dielectric constant of insulating material on entering side of boundary (side of incidence).

where K2=delectric constant of insulating maalamo? ter'ial on other side of boundaryfside of're Vfraction) Thus, it is seen that to secure proper refraction of the wave the angles A and B. are determined by the square root yof the ratio of the dielectric constants for the insulating materials used on each side of the boundary.

In meeting the requirement for constant surge impedane on each side of the boundary, refer-A ence is made to the formula yforsurge impedance already mentioned in which From this equation, itwill be apparent that the surge impedance Z is inversely proportional .to E However, the equation just mentioned is that for the surge impedance of a cylindrical cable. On the other hand, the diagrammatic View of Fig. 7 shows a small rectangular strip of a dielectric medium with conductors on opposite faces. In the equations to follow, the surge impedance for such a small rectangular strip will be de.-l rived from the equation for the Surge impedance of a cylindrical cable.

Referring to Fig. 9, it will be apparent ,from the formula gvenfor the Surge impedance 0f a, cable that r=the radius of the inner conductor r+t=the radius of the outer conductor As angle A in Fig. 9 grows smaller and smaller, the volume of dielectric material contained in the angle will approach a rectangular prism. The anale Aincludes a length a on the circumference ofl circle having radius rso that the surge im. pedante of the volume in angle A is 21r1' 60 l ZA=T 10g. (l +7) Since the quantity 120 isla constant By comparing'Figs. 9 and 7. it will be apparent that the distance tin Fig. corresponda to in Fig. 7. Assuming that Z1=surge impedancev on theenterng side of the boundary 5 Z2=surge impedance on the opposite side of the boundary, then Z =F yio JIT, w/Il VIK: N/Kz 1' ""i Li== DE' cos A zcos B 2Q VKZ" cos'A Since for constant surge impedance E=cos B K2 cos A and for proper refraction of the Wave ijn A Kz-SD B these two` equations may be solved simultaneously to incorporate both factors in determining the ultimate values of angles A and B. Thus .But by the previous-equation u Comparing the two equations sin A=cos B This solution gives values for angles A and B such that Thus it will be seen that'v the boundary angle is determined by the ratio of the dielectric constants of the insulating materials on each side Iof the boundary. For the special case in which air, having a dielectric constant of l, is used on one side of the boundary the expression 1 /I- becomes since K2=l In the showing of Figs. l, 7 and 8, and in the mathematical steps set forth above, the electric wave has been considered as passing from a solid dielectric medium into a gaseous one. This has been done in the interest of simplification and to make the functions of the boundary more clearly apparent. However, it should be realized that the electric wave also travels in a reverse direction, i. e., from the gaseous to the solid dielectric medium. In such instances, the angles A and B in the equations mentioned above would be reversed. Similarly, Z1 and Z2 would be reversed as would K1 and K2.

Turning now to the actual construction of my invention shown by Fig. l, two cable sections I and 2 are joined together with a connector 3. Each cable section has an inner conductor 4 and an outer conductor 5, in the present instance made of braided material and concentrically spaced from the inner conductor 4. The annular space between the conductors is filled with insulating material, in the present example, a solid dielectric 6, such as polyethylene. The outer conductor 5 is protected by a jacket I made from suitable material such as polyvinyl chloride.

The connector 3 for connecting two cable sections i and 2 is made up of two terminals and includes means for securing and electrically connecting such terminals together. Each terminal comprises a casing 8 which has a substantially cylindrical end portion Q, a substantially conical or tapered intermediate portion I and a substantially cylindrical end portionv II. The cylindrical casing portion 9 forms a packingchamber to receive the severed end of the cable. A braid clamp I2 is located in said chamber between an outwardly turned portion of the braided outer conductor and the jacket 'I. The `acket I is securely sealed tothe casing 9 and the outer conductor is securely'connected to the casing 9 by means of suitable packing rings I3 and washers I4 held in position by a gland nut I5 threaded into the casing 9. In this way, the outer conductor 5 is electrically connected to the joint casing 8.

The inner conductor 4 within the end casing II carries a metallic cone I6 which has its apex near the casing portion 9 and its base within the cylindrical -casing portion II. The surface of the cone is roughly parallel to the inner surface of conical intermediate portion I0. Together these elements form tapered surfaces for maintaining approximately uniform surge impedence through the joint as the small diameter conductors of the cable merge with the larger ones of the joint. The metallic cone I6 has an extension I'I with la threaded collar I8. The cone is secured to and electrically connected with the conductor 4 by any suitable means such as solder I9 lling an opening in the cylindrical portion I'I. A sleeve 20 is threaded at one end to the threaded collar I8 of the cone I 6. Each of the two terminals on the two lengths of cable to be connected together has the elements I6 to 2U described above. The sleeves 20 of the two terminals are electrically connected by means of a connecting member 2| which has an end portion 22 disposed within one of the sleeves 2U and preferably brazed or fused thereto. The connecting member 2I has an intermediate portion or collar located between and forming abut-y ments for the adjacent ends of the sleeves 20 of the terminals. The connecting member in addition has a slotted cylindrical portion 23 forming a snug t in the other of the sleeves Z so that a good electrical connection is obtained between the sleeves.

The casings 8 of the terminals are electrically and mechanically securely connected together by a suitable coupling. In the present example, the casing 8 of the left-hand terminal is provided with a flanged extension 24 secured to the casing by suitable means such as solder 25. The casing 8 of the right-hand terminal is provided with another iianged extension 2B suitably secured to the casing. The flanged extensions are sealed together by means including a packing ring 21 and a iianged nut 28. Y

The solid dielectric 6 has a conical end face or boundary 29 and is held in position in tight sealing engagement with the outer conductor or casing by means of a sealing gasket 30 engaging the outer end portion of the solid dielectric and held in position by a retaining ring 3I. The retaining ring itself is held in position by a spun-in' projection 32 of the casing. The sleeves 20 of the two terminals and the intermediate portion'v tain instances, the space 33 might be iilled'with` insulating compound having high dielectric strength, for example, polystyrene.

As aforementioned, the boundary surface 29 makes an angle with the dielectric media of the cable and jointvsu'ch that As shown by Figure 1, the angles A and B are measured from a line normal or perpendicular to the boundaryzline 29 of the solid dielectric material. The solid dielectric as far as it engages directly the cylindrical c onductor 4 has a constant inner diameter. Adjacent the metallic cone I6 the diameter of the solid dielectric increases gradually and reaches a maximum at or E tan AWN/K2 and cot B Preferably, the annular space 33 formed near the base of thefmetallic vcone I6. In other words, the inner surface of the soliddielectric is substantially conical within-the cable connector or terminal and has a tangent approach to the cylindrical inner surface of the solid dielectric in the cable section. The cuter surface of the solid dielectric in the connector is likewise substantially conical with slightlycurved contour and a diameter increasing toward the end of the cable. The inner and outer curvatures of the solid dielectric should be as small as possible. Practical considerations limit the length of the conical surfaces. The outer diameter of the inner cylindrical conductor and the inner diameter of the outer cylindrical conductor of the connector arechosen to produce with the chosen dielectric a uniform surge impedance equal to that of the solid cable section.

If an electric wave is considered approaching the boundary from the solid side, it is desirable, from a theoretical standpoint, that the wave approach the boundary at the angle of incidence B, as indicated in the diagrammatic showing of Fig. 7. If this were to happen, it would mean that the contours of the inner and outer cones of the concentric conductors should approach the boundary at the same angle inY order to vcause the electric wave to approachat the desired. angle. However, from a practical standpoint,v it is not possible to have both the inner and outer cones approach the boundary at the same angle because considerations of substantially constant surge impedance require that the two curves of the cones diverge. Although it is necessary to make the cones'diverge, it is possible to reduce the undesirable effect of the divergence kby making the two conesdiverge from the desired angle of incidence by equal amountsA and lx1-,opposite directions so that the average of the directions of the two cones will be substantiallycorrect. This would mean that the average angle of 'incidence of an electric wave would be correct. The cable joint thus far described, is constructed by the new and improved method and apparatus :comprising my invention.

During manufacture of a cable joint or terminal according to my invention the jacket 1 is stripped back from the end portion of a cable (Fig. 2). Thereupon the gland .nut I5, washers I4 and gaskets I3 are passed over the jacket 1 and the braid clamp I2 is passed over the louter conductor 5 and wedged under the jacket 1. The braid 5, forming the outer conductor of the cable, is then turned outwardly to form a iiange around the braid clamp I2. The casing B is then passed over the cable end portion. The gland nut I5 is tightened to form a weather-proof seal between the casing 8 and the jacket 1 ofthe cable section. In the present instance the inner conductor 4 and the solid dielectric B on the -end portion extend `axially beyond the casing 8,. The terminal parts thus far assembled are then placed into a molding press to'mold the dielectric material on'the end portion into the desired shape.v

The press to accomplisli'this, as vshown in part in Fig. 2 and in full .in Fig.`5, comprises `a cylinder 34 forming a molding chamber. An inletchannel 35 connected to a pipe 36 and-an exhaust port 31 permits a heating medium, such as hot air, to be circulated in the cylinder 34 during the molding operation. vThe cylinder' 34 hasazthreaded end portion mounted on a supporting platei38 and forming'an inner annular shoulder 39. The supporting plate, 38.15 .connected v.toian end plate 40 (Fig. 5) by means of four rods 4I. A plunger 42 is slidable into the right-hand end oi the cylinder 34 and has an end face 43 which conforms to the predetermined shape of the boundary or end face 29 (Fig. 1) to be produced. The plunger has a vent channel 44 for discharging gases as the plunger passes beyond the exhaust opening 3'1 and for discharging some of the molded dielectric compound during the molding operation (Fig. 3), for a purpose to be described later.

As shown by Figure 5, the right-hand end of the plunger is secured to a threaded sleeve 45 and a plate 46 slidably engaging the rods 4I and acting as a guide for the plunger on said rods. The plunger is actuated, that is, moved axially by means of al screw 41 connected at its right-hand end to a handle 48 and having screw engagement with the end plate 49. The left-hand end of the screw 41 has a head 49 supported within the sleeve 45 by means of a ball-bearing 50 and is loosely connected to the plunger 42 by a slidable cup 5I and a compression spring 52. Upon clockwise rotation of the handle 48 the screw 41 is moved toward the left. This movement is transmitted through the spring 52 to the plunger 42. The spring normally acts as a shock absorber to effect uniform transmission of force from the screw to the cylinder. As the resistance to movement of the plunger increases during the molding operation the spring is compressed until the cup 5I engages directly the end face of the plunger 42, the spring then being completely enclosed within a bore in the plunger.

The left-hand end of the plunger 42 has a shoulder 53 for supporting the base of the metallic cone I6. In some instances it may be desirable to use a special steel cone of same shape as the cone I6 for the molding operation. During the molding operation a cone I6 is inserted into the end of the plunger and a cable with aterrninal casing is assembled on the tool as shown in Figs. 2 and 5. The casing 8 of the terminal is then seated against the shoulder 39 of the cylinder 34.

As shown in the exploded View of Fig. 6, the molding press includes means for clamping in position a cable with a terminal casing thereon. This means includes a cylinder 54 having a threaded portion secured to an anchor plate 55 held on the supporting plate 38 by means of two spaced rods 56. The cable projects centrally through the cylinder and is engaged by means of a three-part clamp 51 bearing against a thrust plate 58 provided with a conical opening 59. The thrust plate is seated against the right-hand end of the cylinder 54 and has an opening 50 for accommodating one of the rods 55 and a recess 6I for accommodating the other rod 56. The rod 55 projects through the opening 60 of the thrust plate and constitutes a pivot for the latter; that is, the thrust plate may be swung into position about the rod 56 so that the other rod 58 Slips into the recess SI.

During assembly a cable with a terminal casing thereon is inserted through the cylinder 54. Thereupon the three parts of the clamp 51 are positioned about the cable. Then the thrust plate 58 is moved into positionto support the clamp and finally thethreaded cylinder 54 is rotated toward the thrust plate 58 in order to force the thrust plate 58 up around the'clamp which, in turn, engages theterminal casing.

During construction of the joint, it is desirable vto strip the cable in a manner such that the amount of compound lei-t on the end portion is slnlcientto'produce the enlarged conical end portion of the dielectric. Income cases where lthe Volume of compound on the end of the conductor is not suicient, additional compound may be placed into the casing in the form of a ring or insulation pellet 62 as shown in Fig. 4. This additional compound is to be of the same dielectric material as that on the cable.

During the molding operation, hot air or like heating medium, is admitted through the pipe V36 to the cylinder 34 to heat the insulation until it reaches a certain temperature, for example, 110 C. in case such insulation or dielectric is made from polyethylene. Thereupon the plunger 42 is slowly advanced by rotating the handle 48. As the plunger advances, the cone i6 peels back the dielectric medium on the cable, and together with the angular end face 43 on the plunger, forces the insulation into the tapered section l of the terminal casing.

Although the molding press and the dielectric compound on the cable are heated during the initial stages of the molding operation, it is imf portant that the dielectric compound be completely cooled upon completion of the operation.

This is so because the dielectric, such as polyethylene, contracts upon cooling and it is extremely important that there be no voids in the dielectric compound after it has been molded into position. For this reason, during the latter stages of the molding operation, the terminal and molding press near the cable end of the construction are cooled by means of a water bath.

Since the dielectric compound shrinks on cooling, it is important for the operator to know Whether or not the plunger of the molding press is being moved fast enough to make up for any shrinkage in the compound to prevent the formation of voids. This is the purpose of the channel 44. As the plunger is advanced, compound is forced out through the passage 44, in the manner indicated by Fig. 3. If the excess compound were allowed to creep out of the molding press along clearances between the plunger 42 and the cylinder 34, the operator would not be sure that the plunger was being advanced at the proper rate because a considerable amount of the dielectric compound might accumulate out of sight in the space between these two members. However, by providing the channel 44, the operator can immediately ascertain whether or not the plunger is being moved at the proper rate because the excess compound is always visible.

During the molding operation, the operator should move the plunger 42 fast enough so that material is continuously extruded through the channel 44 during the entire molding cycle. Moreover, it will be apparent that the rate at which material is extruded out of the channel 44 will give the operator an indication as to whether or not the plunger is being moved at the proper speed. If the plunger is moved too fast during the initial stages of the molding cycle, then an excess of dielectric compound will be extruded through the channel 44 giving an indication to the operator to decrease the speed of the plunger. On the other hand, during the latter stages of the molding cycle when the dielectric compound is being cooled down and shrunk, if no compound is extruded through the channel 44, then the operator will know that the plunger 42 is not being advanced fast enough. Under ideal conditions, the press should be operated in such a way that the plunger reaches its nal position at a time when the insulation has become thoroughly cooled and shrunk and "the plunger' should Vbe operated so that the'dielectric compound is extruded through the channel 44 continuously during movement of the plunger. When this procedure is followed, it is practically certain that there will be no voids in the molded insulation of the terminal.

Upon completion of the molding operation, the terminal casing is removed from the press and the gasket 30 is inserted together with the retaining ring 3|. The gasket 30 is held in position by application of pressure on the retaining ring and then a projection isspun in the cylindrical casing 8 to hold the retaining ring 3| in position. The projection 32 may be formed by rotating the terminal casing on a mandrel. Alternatively, the terminal casing may be held fast and a suitable forming tool rotated around the periphery of the casing. Finally, the metal cone I6 is secured to the inner conductor by any suitable means such as the solder I9. Then the coupling member 24 or 26 is fastened to the terminal casing 8.

Thus, with my invention I have accomplished an improved method for making cable connectors -in which reection of high frequency waves in the cable is substantially eliminated and whereby the' characteristic or surge impedance remains substantially constant throughout the cable lengths and joint. The method of attaching the connectors to the cable isA one which may be performed equally as well in the field as in the factory. Connectors constructed in accordance with my invention are simple in construction and are especially suitable for making joints in field use.

While I have shown and described a particular embodiment of my invention, other changes and modiiications will be obvious to'those skilled in the art and I','therefore, aim in the appended claims to cover all such changes and modifications as fallwithin the true spiritand scope o my invention.

What I claim as new and desire to secure by Letters Patent of the United States, is:

1. A method of forming a terminal on a cable having concentric conductors separated by a solid dielectric which comprises the steps of removing the outer conductor from an end portion of said cable, securing a terminal casing to the outer conductor, placing a contact member on the inner conductor, applying heat to the interior of said casing to Vsoften the dielectric on said end portion and then simultaneously moving said contact member along the inner conductor to strip the softened dielectric therefrom, molding the stripped insulation in said casing and cooling said stripped insulation being molded.

2. The method of forming a terminal on a cable having concentric conductors separated by a solid dielectric which comprises removing the outer conductor from an end portion of said cable, securing a terminal casing to the outer conductor, placing' a contact member on the inner conductor, applying heat to the interior of said casing to soften the dielectric on said end portion, moving said contact member along the inner conductor to strip the softened dielectric therefrom and simultaneously molding the stripped insulation in said casing, cooling the insulation as it is being molded and ejecting excess stripped insulation continuously from said casing until termination of said molding operation.

LYNN WETHERILL.

(References on following page) REFERENCES CITED The following references are of record in the file of this patent:

UNITED STATES PATENTS Number Name Date McIntire July 3, 1900 Green Dec. 5. 1933 Number 

